Physics Working Formulas

PHYSICS FORMULAS
2426
Electron = -1.602 19 × 10-19
C = 9.11 × 10-31 kg
Proton = 1.602 19 × 10-19
C = 1.67 × 10-27 kg
Neutron = 0 C = 1.67 × 10-27 kg
6.022 × 1023
atoms in one atomic mass unit
e is the elementary charge: 1.602 19 × 10-19
C
Potential Energy, velocity of electron: PE = eV = ½mv2
1V = 1J/C 1N/C = 1V/m 1J = 1 N·m = 1 C·V
1 amp = 6.21 × 1018
electrons/second = 1 Coulomb/second
1 hp = 0.756 kW 1 N = 1 T·A·m 1 Pa = 1 N/m2
Power = Joules/second = I2
R = IV [watts W]
Quadratic
Equation: x
b b ac
a
=
− ± −2
4
2
Kinetic Energy [J]
KE mv= 1
2
2
[Natural Log: when eb
= x, ln x = b ]
m: 10
-3
µ: 10
-6
n: 10
-9
p: 10
-12
f: 10
-15
a: 10
-18
Addition of Multiple Vectors:
r r r r
R A B C= + + Resultant = Sum of the vectorsr r r r
R A B Cx x x x= + + x-component A Ax = cos θ
r r r r
R A B Cy y y y= + + y-component A Ay = sin θ
R R Rx y= +2 2
Magnitude (length) of R
θR
y
x
R
R
= −
tan 1
or tanθR
y
x
R
R
= Angle of the resultant
Multiplication of Vectors:
Cross Product or Vector Product:
i j k× = j i k× = −
i i× = 0
Positive direction:
i
j k
Dot Product or Scalar Product:
i j⋅ = 0 i i⋅ = 1
a b⋅ = abcosθ
k
i
j
Derivative of Vectors:
Velocity is the derivative of position with respect to time:
v k i j k= + + = + +
d
dt
x y z
dx
dt
dy
dt
dz
dt
( )i j
Acceleration is the derivative of velocity with respect to
time:
a k i j k= + + = + +
d
dt
v v v
dv
dt
dv
dt
dv
dtx y z
x y z
( )i j
Rectangular Notation: Z R jX= ± where +j represents
inductive reactance and -j represents capacitive reactance.
For example, Z j= +8 6Ω means that a resistor of 8Ω is
in series with an inductive reactance of 6Ω.
Polar Notation: Z = M ∠θ, where M is the magnitude of the
reactance and θ is the direction with respect to the
horizontal (pure resistance) axis. For example, a resistor of
4Ω in series with a capacitor with a reactance of 3Ω would
be expressed as 5 ∠-36.9° Ω.
In the descriptions above, impedance is used as an example.
Rectangular and Polar Notation can also be used to
express amperage, voltage, and power.
To convert from rectangular to polar notation:
Given: X - jY (careful with the sign before the ”j”)
Magnitude: X Y M2 2
+ =
Angle:
tanθ =
− Y
X
(negative sign carried over
from rectangular notation
in this example)
Note: Due to the way the calculator works, if X is negative,
you must add 180° after taking the inverse tangent. If the
result is greater than 180°, you may optionally subtract
360° to obtain the value closest to the reference angle.
To convert from polar to rectangular (j) notation:
Given: M ∠θ
X Value: M cosθ
Y (j) Value: M sinθ
In conversions, the j value will have the
same sign as the θ value for angles
having a magnitude < 180°.
Use rectangular notation when adding
and subtracting.
Use polar notation for multiplication and division. Multiply in
polar notation by multiplying the magnitudes and adding
the angles. Divide in polar notation by dividing the
magnitudes and subtracting the denominator angle from
the numerator angle.
X
MMagnitude
θ
Y

ELECTRIC CHARGES AND FIELDS
Coulomb's Law: [Newtons N]
F k
q q
r
= 1 2
2
where: F = force on one charge by
the other[N]
k = 8.99 × 109 [N·m2/C2]
q1 = charge [C]
q2 = charge [C]
r = distance [m]
Electric Field: [Newtons/Coulomb or Volts/Meter]
E k
q
r
F
q
= =2
where: E = electric field [N/C or V/m]
k = 8.99 × 109 [N·m2/C2]
q = charge [C]
r = distance [m]
F = force
Electric field lines radiate outward from
positive charges. The electric field
is zero inside a conductor.
+ -
Relationship of k to ∈∈0:
k =
∈
1
4 0π
where: k = 8.99 × 109 [N·m2/C2]
∈0 = permittivity of free space
8.85 × 10-12 [C2/N·m2]
Electric Field due to an Infinite Line of Charge: [N/C]
E
r
k
r
=
∈
=
λ
π
λ
2
2
0
E = electric field [N/C]
λ = charge per unit length [C/m}
8.85 × 10-12 [C2/N·m2]
r = distance [m]
k = 8.99 × 109 [N·m2/C2]
Electric Field due to ring of Charge: [N/C]
E
kqz
z R
=
+( ) /2 2 3 2
or if z >> R, E
kq
z
= 2
k = 8.99 × 109 [N·m2/C2]
q = charge [C]
z = distance to the charge [m]
R = radius of the ring [m]
Electric Field due to a disk Charge: [N/C]
E
z
z R
=
∈
−
+






σ
2
1
0
2 2
σ = charge per unit area
[C/m
2
}
∈0 = 8.85 × 10-12 [C2
/N·m2
]
z = distance to charge [m]
R = radius of the ring [m]
Electric Field due to an infinite sheet: [N/C]
E =
∈
σ
2 0
σ = charge per unit area [C/m
2
}
∈0 = 8.85 × 10-12 [C2
/N·m2
]
Electric Field inside a spherical shell: [N/C]
E
kqr
R
= 3
q = charge [C]
r = distance from center of sphere to
the charge [m]
R = radius of the sphere [m]
Electric Field outside a spherical shell: [N/C]
E
kq
r
= 2
q = charge [C]
r = distance from center of sphere to
the charge [m]
Average Power per unit area of an electric or
magnetic field:
W m
E
c
B cm m
/ 2
2
0
2
02 2
= =
µ µ
W = watts
Em = max. electric field [N/C]
µ0 = 4π × 10-7
c = 2.99792 × 108
[m/s]
Bm = max. magnetic field [T]
A positive charge moving in the same direction as the electric
field direction loses potential energy since the potential of
the electric field diminishes in this direction.
Equipotential lines cross EF lines at right angles.
Electric Dipole: Two charges of equal magnitude and
opposite polarity separated by a distance d.
z
-Q
p
d
+Q
E
k
z
=
2
3
p
E
z
=
∈
1
2 0
3
π
p
when z » d
k = 8.99 × 109 [N·m2/C2]
∈0 = permittivity of free space 8.85 ×
10-12 C2/N·m2
p = qd [C·m] "electric dipole moment"
in the direction negative to
positive
z = distance [m] from the dipole
center to the point along the
dipole axis where the electric field
is to be measured
Deflection of a Particle in an Electric Field:
2 2 2
ymv qEL=
y = deflection [m]
m = mass of the particle [kg]
d = plate separation [m]
v = speed [m/s]
q = charge [C]
E = electric field [N/C or V/m
L = length of plates [m]

Potential Difference between two Points: [volts V]
∆
∆
V V V
PE
q
EdB A= − = = −
∆PE = work to move a charge
from A to B [N·m or J]
q = charge [C]
VB = potential at B [V]
VA = potential at A [V]
E = electric field [N/C or V/m
d = plate separation [m]
Electric Potential due to a Point Charge: [volts V]
V k
q
r
=
V = potential [volts V]
k = 8.99 × 109 [N·m2/C2]
q = charge [C]
r = distance [m]
Potential Energy of a Pair of Charges: [J, N·m or
C·V]
PE q V k
q q
r
= =2 1
1 2
V1 is the electric potential due to
q1 at a point P
q2V1 is the work required to bring
q2 from infinity to point P
Work and Potential:
∆U U U Wf i= − = −
U W= − ∞
W Fd= ⋅ =F d cosθ
W q d
i
f
= ⋅∫E s
∆V V V
W
qf i= − = −
V d
i
f
= − ⋅∫E s
U = electric potential energy [J]
W = work done on a particle by
a field [J]
W∞ = work done on a particle
brought from infinity (zero
potential) to its present
location [J]
F = is the force vector [N]
d = is the distance vector over
which the force is
applied[m]
F = is the force scalar [N]
d = is the distance scalar [m]
θ = is the angle between the
force and distance vectors
ds = differential displacement of
the charge [m]
V = volts [V]
q = charge [C]
Flux: the rate of flow (of an electric field) [N·m2
/C]
Φ = ⋅∫E Ad
= ∫ E dA(cos )θ
ΦΦ is the rate of flow of an electric
field [N·m
2
/C]
∫ integral over a closed surface
E is the electric field vector [N/C]
A is the area vector [m
2
] pointing
outward normal to the surface.
Gauss' Law:
∈ =0 Φ qenc
∈ ⋅ =∫0 E Ad qenc
∈0 = 8.85 × 10-12 [C2
/N·m2
]
ΦΦ is the rate of flow of an electric
field [N·m2
/C]
qenc = charge within the gaussian
surface [C]
∫ integral over a closed surface
E is the electric field vector [J]
A is the area vector [m2
] pointing
outward normal to the surface.
CAPACITANCE
Parallel-Plate Capacitor:
C
A
d
= ∈κ 0
C = capacitance [farads F]
κ = the dielectric constant (1)
8.85 × 10-12 C2/N·m2
A = area of one plate [m2]
d = separation between plates [m]
Cylindrical Capacitor:
C
L
b a
= ∈2 0πκ
ln( / )
κ = dielectric constant (1)
∈0 = 8.85 × 10
-12
C2/N·m2
L = length [m]
b = radius of the outer
conductor [m]
a = radius of the inner
conductor [m]
Spherical Capacitor:
C
ab
b a
= ∈
−
4 0πκ
κ = dielectric constant (1)
∈0 = 8.85 × 10
-12
C2/N·m2
b = radius, outer conductor
[m]
a = radius, inner conductor [m]
Maximum Charge on a Capacitor: [Coulombs C]
Q VC= Q = Coulombs [C]
V = volts [V]
C = capacitance in farads [F]
For capacitors connected in series, the charge Q is equal for
each capacitor as well as for the total equivalent. If the
dielectric constant κ is changed, the capacitance is
multiplied by κ, the voltage is divided by κ, and Q is
unchanged. In a vacuum κ = 1, When dielectrics are
used, replace ∈0 with κ ∈0.
Electrical Energy Stored in a Capacitor: [Joules J]
U
QV CV Q
CE = = =
2 2 2
2 2 U = Potential Energy [J]
Q = Coulombs [C]
V = volts [V]

Charge per unit Area: [C/m2
]
σ =
q
A
σ = charge per unit area [C/m2
]
q = charge [C]
A = area [m2
]
Energy Density: (in a vacuum) [J/m3
]
u E= ∈1
2 0
2 u = energy per unit volume [J/m3
]
8.85 × 10-12 C2/N·m2
E = energy [J]
Capacitors in Series:
1 1 1
1 2C C Ceff
= + ...
Capacitors in Parallel:
C C Ceff = +1 2 ...
Capacitors connected in series all have the same charge q.
For parallel capacitors the total q is equal to the sum of the
charge on each capacitor.
Time Constant: [seconds]
τ = RC τ = time it takes the capacitor to reach 63.2%
of its maximum charge [seconds]
R = series resistance [ohms Ω]
Charge or Voltage after t Seconds: [coulombs C]
charging:
( )q Q e t
= − −
1 /τ
( )V V eS
t
= − −
1 /τ
discharging:
q Qe t
= − /τ
V V eS
t
= − /τ
q = charge after t seconds
[coulombs C]
Q = maximum charge [coulombs
C] Q = CV
e = natural log
t = time [seconds]
τ = time constant RC [seconds]
V = volts [V]
VS = supply volts [V]
[Natural Log: when eb
= x, ln x = b ]
Drift Speed:
( )I
Q
t
nqv Ad= =
∆
∆
∆Q = # of carriers × charge/carrier
∆t = time in seconds
n = # of carriers
q = charge on each carrier
vd = drift speed in meters/second
A = cross-sectional area in meters
2
RESISTANCE
Emf: A voltage source which can provide continuous current
[volts]
ε = +IR Ir ε = emf open-circuit voltage of the battery
I = current [amps]
R = load resistance [ohms]
r = internal battery resistance [ohms]
Resistivity: [Ohm Meters]
ρ =
E
J
ρ =
RA
L
ρ = resistivity [Ω · m]
J = current density [A/m2
]
R = resistance [Ω ohms]
A = area [m2
]
L = length of conductor [m]
Variation of Resistance with Temperature:
ρ ρ ρ α− = −0 0 0( )T T ρ = resistivity [Ω · m]
ρ0 = reference resistivity [Ω · m]
α = temperature coefficient of
resistivity [K-1
]
T0 = reference temperature
T - T0 = temperature difference
[K or °C]
CURRENT
Current Density: [A/m
2
]
i d= ⋅∫J A
if current is uniform
and parallel to dA,
then: i JA=
J ne Vd= ( )
i = current [A]
J = current density [A/m
2
]
A = area [m
2
]
L = length of conductor [m]
e = charge per carrier
ne = carrier charge density [C/m
3
]
Vd = drift speed [m/s]
Rate of Change of Chemical Energy in a Battery:
P i= ε P = power [W]
i = current [A]
ε = emf potential [V]
Kirchhoff’s Rules
1. The sum of the currents entering a junctions is equal to
the sum of the currents leaving the junction.
2. The sum of the potential differences across all the
elements around a closed loop must be zero.
Evaluating Circuits Using Kirchhoff’s Rules
1. Assign current variables and direction of flow to all
branches of the circuit. If your choice of direction is
incorrect, the result will be a negative number. Derive
equation(s) for these currents based on the rule that
currents entering a junction equal currents exiting the
junction.
2. Apply Kirchhoff’s loop rule in creating equations for
different current paths in the circuit. For a current path
beginning and ending at the same point, the sum of
voltage drops/gains is zero. When evaluating a loop in the
direction of current flow, resistances will cause drops
(negatives); voltage sources will cause rises (positives)
provided they are crossed negative to positive—otherwise
they will be drops as well.
3. The number of equations should equal the number of
variables. Solve the equations simultaneously.

MAGNETISM
André-Marie Ampére is credited with the discovery of
electromagnetism, the relationship between electric
currents and magnetic fields.
Heinrich Hertz was the first to generate and detect
electromagnetic waves in the laboratory.
Magnetic Force acting on a charge q: [Newtons N]
F qvB= sinθ
F q= ×v B
F = force [N]
q = charge [C]
v = velocity [m/s]
B = magnetic field [T]
θ = angle between v and B
Right-Hand Rule: Fingers represent the direction of the
magnetic force B, thumb represents the direction of v (at
any angle to B), and the force F on a positive charge
emanates from the palm. The direction of a magnetic field
is from north to south. Use the left hand for a negative
charge.
Also, if a wire is grasped in the right hand with the thumb in
the direction of current flow, the fingers will curl in the
direction of the magnetic field.
In a solenoid with current flowing in the direction of curled
fingers, the magnetic field is in the direction of the thumb.
When applied to electrical flow caused by a changing
magnetic field, things get more complicated. Consider the
north pole of a magnet moving toward a loop of wire
(magnetic field increasing). The thumb represents the
north pole of the magnet, the fingers suggest current flow in
the loop. However, electrical activity will serve to balance
the change in the magnetic field, so that current will
actually flow in the opposite direction. If the magnet was
being withdrawn, then the suggested current flow would be
decreasing so that the actual current flow would be in the
direction of the fingers in this case to oppose the decrease.
Now consider a cylindrical area of magnetic field going into
a page. With the thumb pointing into the page, this would
suggest an electric field orbiting in a clockwise direction. If
the magnetic field was increasing, the actual electric field
would be CCW in opposition to the increase. An electron in
the field would travel opposite the field direction (CW) and
would experience a negative change in potential.
Force on a Wire in a Magnetic Field: [Newtons N]
F BI= lsinθ
F I B= ×l
F = force [N]
I = amperage [A]
l = length [m]
θ = angle between B and the
direction of the current
Torque on a Rectangular Loop: [Newton·meters N·m]
τ θ= NBIAsin N = number of turns
I = amperage [A]
A = area [m
2
]
plane of the loop
Charged Particle in a Magnetic Field:
r
mv
qB
=
r = radius of rotational path
m = mass [kg]
v = velocity [m/s]
q = charge [C]
Magnetic Field Around a Wire: [T]
B
I
r
=
µ
π
0
2
µ0 = the permeability of free
space 4π×10-7
T·m/A
I = current [A]
r = distance from the center of
the conductor
Magnetic Field at the center of an Arc: [T]
B
i
r
=
µ φ
π
0
4
space 4π×10-7
T·m/A
i = current [A]
φ = the arc in radians
r = distance from the center of
the conductor
Hall Effect: Voltage across the width of a
conducting ribbon due to a Magnetic Field:
( )ne V h Biw =
v Bw Vd w=
ne = carrier charge density [C/m
3
]
Vw = voltage across the width [V]
h = thickness of the conductor [m]
i = current [A]
vd = drift velocity [m/s]
w = width [m]
Force Between Two Conductors: The force is
attractive if the currents are in the same direction.
F I I
d
1 0 1 2
2l
=
µ
π
F = force [N]
l = length [m]
space 4π×10
-7
T·m/A
I = current [A]
d = distance center to center [m]
Magnetic Field Inside of a Solenoid: [Teslas T]
B nI= µ0
space 4π×10
-7
T·m/A
n = number of turns of wire per
unit length [#/m]
I = current [A]
Magnetic Dipole Moment: [J/T]
µ = NiA µ = the magnetic dipole moment [J/T]
N = number of turns of wire
i = current [A]
A = area [m2
]
Magnetic Flux through a closed loop: [T·M
2
or Webers]
Φ = BAcosθ B = magnetic field [T]
A = area of loop [m
2
]
perpen-dicular to the plane of
the loop

Magnetic Flux for a changing magnetic field: [T·M2
or
Webers]
Φ = ⋅∫B Ad
A = area of loop [m2
]
A Cylindrical Changing Magnetic Field
E s⋅ = =∫ d E r
d
dt
B
2π
Φ
ΦB BA B r= = π 2
d
dt
A
dB
dt
Φ
=
ε = −N
d
dt
Φ
r = radius [m]
t = time [s]
Φ = magnetic flux [T·m2
or
Webers]
A = area of magnetic field
[m2
]
dB/dt = rate of change of
the magnetic field [T/s]
ε = potential [V]
N = number of orbits
Faraday’s Law of Induction states that the instan-
taneous emf induced in a circuit equals the rate of
change of magnetic flux through the circuit. Michael
Faraday made fundamental discoveries in
magnetism, electricity, and light.
ε = −N
t
∆Φ
∆
N = number of turns
Φ = magnetic flux [T·m
2
]
t = time [s]
Lenz’s Law states that the polarity of the induced emf is
such that it produces a current whose magnetic field
opposes the change in magnetic flux through a circuit
Motional emf is induced when a conducting bar moves
through a perpendicular magnetic field.
ε = B vl B = magnetic field [T]
l = length of the bar [m]
v = speed of the bar [m/s]
emf Induced in a Rotating Coil:
ε ω ω= NAB tsin N = number of turns
A = area of loop [m
2
]
ω = angular velocity [rad/s]
t = time [s]
Self-Induced emf in a Coil due to changing current:
ε = −L
I
t
∆
∆
L = inductance [H]
I = current [A]
t = time [s]
Inductance per unit length near the center of a solenoid:
L
n A
l
= µ0
2
L = inductance [H]
l = length of the solenoid [m]
µ0 = the permeability of free space
4π×10-7
T·m/A
n = number of turns of wire per unit
length [#/m]
A = area [m
2
]
Amperes' Law:
B s⋅ =∫ d iencµ0
µ0 = the permeability of free space
4π×10-7
T·m/A
ienc = current encircled by the
loop[A]
Joseph Henry, American physicist, made improvements
to the electromagnet.
James Clerk Maxwell provided a theory showing the
close relationship between electric and magnetic
phenomena and predicted that electric and magnetic
fields could move through space as waves.
J. J. Thompson is credited with the discovery of the
electron in 1897.
INDUCTIVE & RCL CIRCUITS
Inductance of a Coil: [H]
L
N
I
=
Φ N = number of turns
Φ = magnetic flux [T·m2
]
I = current [A]
In an RL Circuit, after one time constant (τ = L/R) the
current in the circuit is 63.2% of its final value, ε/R.
RL Circuit:
current rise:
( )I
V
R
e t L
= − −
1 /τ
current decay:
I
V
R
e t L
= − /τ
UB = Potential Energy [J]
V = volts [V]
R = resistance [Ω]
e = natural log
t = time [seconds]
τL = inductive time constant L/R
[s]
I = current [A]
Magnetic Energy Stored in an Inductor:
U LIB = 1
2
2 UB = Potential Energy [J]
L = inductance [H]
I = current [A]
Electrical Energy Stored in a Capacitor: [Joules J]
U
QV CV Q
CE = = =
2 2 2
2 2 UE = Potential Energy [J]
Q = Coulombs [C]
V = volts [V]
Resonant Frequency: : The frequency at which XL = XC.
In a series-resonant circuit, the impedance is at its
minimum and the current is at its maximum. For a
parallel-resonant circuit, the opposite is true.
f
LC
R =
1
2π
ω =
1
LC
fR = Resonant Frequency [Hz]
L = inductance [H]
ω = angular frequency [rad/s]

Voltage, series circuits: [V]
V
q
CC = V IRR =
V
X
V
R
IX R
= =
V V VR X
2 2 2
= +
VC = voltage across capacitor [V]
q = charge on capacitor [C]
fR = Resonant Frequency [Hz]
L = inductance [H]
I = current [A]
V = supply voltage [V]
VX = voltage across reactance [V]
VR = voltage across resistor [V]
Phase Angle of a series RL or RC circuit: [degrees]
tanφ = =
X
R
V
V
X
R
cosφ = =
V
V
R
Z
R
(φ would be negative
in a capacitive circuit)
φ = Phase Angle [degrees]
X = reactance [Ω]
VR = voltage across resistor [V]
Z = impedance [Ω]
Impedance of a series RL or RC circuit: [Ω]
Z R X2 2 2
= +
E I Z=
Z
V
X
V
R
V
C
C R
= =
Z R X= ± j
φ = Phase Angle [degrees]
X = reactance [Ω]
VX = voltage across resistor [V]
Z = impedance [Ω]
Series RCL Circuits:
The Resultant Phasor X X XL C= − is
in the direction of the larger reactance
and determines whether the circuit is
inductive or capacitive. If XL is larger
than XC, then the circuit is inductive
and X is a vector in the upward
direction.
In series circuits, the amperage is the
reference (horizontal) vector. This is
observed on the oscilloscope by
looking at the voltage across the
resistor. The two vector diagrams at
right illustrate the phase relationship
between voltage, resistance, reactance,
and amperage.
XC
XL
I
R
VL
CV
I
RV
Series RCL
Impedance Z R X XL C
2 2 2
= + −( ) Z
R
=
cosφ
Impedance may be found by adding the components using
vector algebra. By converting the result to polar notation,
the phase angle is also found.
For multielement circuits, total each resistance and reactance
before using the above formula.
Damped Oscillations in an RCL Series Circuit:
q Qe tRt L
= ′ +− /
cos( )2
ω φ
where
′ = −ω ω 2 2
2( / )R L
ω = 1/ LC
When R is small and ω′ ≈ ω:
U
Q
C
e Rt L
= −
2
2
/
q = charge on capacitor [C]
Q = maximum charge [C]
e = natural log
L = inductance [H]
ω = angular frequency of the
undamped oscillations
[rad/s]
ω = angular frequency of the
damped oscillations
[rad/s]
U = Potential Energy of the
capacitor [J]
Parallel RCL Circuits:
I I I IT R C L= + −2 2
( )
tanφ =
−I I
I
C L
R
V
IL
I
R
C
I
To find total current and phase angle in multielement circuits,
find I for each path and add vectorally. Note that when
converting between current and resistance, a division will
take place requiring the use of polar notation and resulting
in a change of sign for the angle since it will be divided into
(subtracted from) an angle of zero.
Equivalent Series Circuit: Given the Z in polar notation of a
parallel circuit, the resistance and reactance of the
equivalent series circuit is as follows:
R ZT= cosθ X ZT= sinθ
AC CIRCUITS
Instantaneous Voltage of a Sine Wave:
V V ft= max sin2π
V = voltage [V]
f = frequency [Hz]
t = time [s]
Maximum and rms Values:
I
Im
=
2
V
Vm
=
2
I = current [A]
V = voltage [V]
RLC Circuits:
V V V VR L C= + −2 2
( ) Z R X XL C= + −2 2
( )
tanφ =
−X X
R
L C P IVavg = cosφ
PF = cosφ
Conductance (G): The
reciprocal of resistance in
siemens (S).
Susceptance (B, BL, BC): The
reciprocal of reactance in
siemens (S).
Admittance (Y): The reciprocal
of impedance in siemens (S).
YB
Susceptance
Conductance
Admittance
G

ELECTROMAGNETICS
WAVELENGTH
fc λ=
BEc /=
1Å= 10-10
m
c = speed of light 2.998 × 108
m/s
λ = wavelength [m]
f = frequency [Hz]
Å= (angstrom) unit of wavelength
equal to 10-10
m
m = (meters)
WAVELENGTH SPECTRUM
BAND METERS ANGSTROMS
Longwave radio 1 - 100 km 1013
- 1015
Standard Broadcast 100 - 1000 m 1012
- 1013
Shortwave radio 10 - 100 m 1011
- 1012
TV, FM 0.1 - 10 m 109
- 1011
Microwave 1 - 100 mm 107
- 109
Infrared light 0.8 - 1000 µm 8000 - 107
Visible light 360 - 690 nm 3600 - 6900
violet 360 nm 3600
blue 430 nm 4300
green 490 nm 4900
yellow 560 nm 5600
orange 600 nm 6000
red 690 nm 6900
Ultraviolet light 10 - 390 nm 100 - 3900
X-rays 5 - 10,000 pm 0.05 - 100
Gamma rays 100 - 5000 fm 0.001 - 0.05
Cosmic rays < 100 fm < 0.001
Intensity of Electromagnetic Radiation [watts/m
2
]:
I
P
r
s
=
4 2
π
I = intensity [w/m
2
]
Ps = power of source [watts]
r = distance [m]
4πr
2
= surface area of sphere
Force and Radiation Pressure on an object:
a) if the light is totally
absorbed:
F
IA
c
= P
I
cr =
b) if the light is totally
reflected back along the
path:
F
IA
c
=
2
P
I
cr =
2
F = force [N]
I = intensity [w/m
2
]
A = area [m
2
]
Pr = radiation pressure [N/m2
]
c = 2.99792 × 108
[m/s]
Poynting Vector [watts/m2
]:
S EB E= =
1 1
0 0
2
µ µ
cB E=
space 4π×10-7
T·m/A
E = electric field [N/C or V/M]
c = 2.99792 × 108
[m/s]
LIGHT
Indices of Refraction: Quartz: 1.458
Glass, crown 1.52
Glass, flint 1.66
Water 1.333
Air 1.000 293
Angle of Incidence: The angle measured from the
perpendicular to the face or from the perpendicular to the
tangent to the face
Index of Refraction: Materials of greater density have
a higher index of refraction.
n
c
v
≡
n = index of refraction
c = speed of light in a vacuum 3 × 10
8
m/s
v = speed of light in the material [m/s]
n
n
=
λ
λ
0 λ0 = wavelength of the light in a vacuum [m]
λν = its wavelength in the material [m]
Law of Refraction: Snell’s Law
n n1 1 2 2sin sinθ θ= n = index of refraction
θ = angle of incidence
traveling to a region of
lesser density: θ θ2 1>
refracted
Source
n
θ
n1n1
2
1
θ2
traveling to a region of
greater density:
θ θ2 1<
refracted
Source
n
θ
n1n1
2
1
θ2
Critical Angle: The maximum
angle of incidence for which light
can move from n1 to n2
sinθc
n
n
= 2
1
for n1 > n2
Sign Conventions: When M is
negative, the image is inverted. p is positive when the
object is in front of the mirror, surface, or lens. Q is
positive when the image is in front of the mirror or in back
of the surface or lens. f and r are positive if the center of
curvature is in front of the mirror or in back of the surface
or lens.
Magnification by spherical mirror or thin lens. A
negative m means that the image is inverted.
M
h
h
i
p
=
′
= −
h’ = image height [m]
h = object height [m]
i = image distance [m]
p = object distance [m]
reflected
refracted
θ
Source
θ
n1n1
n2

Plane Refracting Surface:
plane refracting surface:
n
p
n
i
1 2
= −
p = object distance
Lensmaker’s Equation for a thin lens in air:
( )
1 1 1
1
1 1
1 2f p i
n
r r
= + = − −






r1 = radius of surface nearest the
object[m]
r2 = radius of surface nearest the
image [m]
f = focal length [m]
p = object distance [m]
Virtual Image
C2
r2
F1
r1
F2 C1
C2
F1
p
F2
i
C1
Real Image
Thin Lens when the thickest part is thin compared to p.
i is negative on the left, positive on the right
f
r
=
2
f = focal length [m]
r = radius [m]
Converging Lens
f is positive (left)
r1 and r2 are positive in
this example
Diverging Lens
f is negative (right)
r1 and r2 are negative in
this example
Two-Lens System Perform the calculation in steps.
Calculate the image produced by the first lens, ignoring the
presence of the second. Then use the image position
relative to the second lens as the object for the second
calculation ignoring the first lens.
Spherical Refracting Surface This refers to two
materials with a single refracting surface.
n
p
n
i
n n
r
1 2 2 1
+ =
−
M
h
h
n i
n p
=
′
= − 1
2
p = object distance
i = image distance [m] (positive for real
images)
f = focal point [m]
r = radius [m] (positive when facing a
convex surface, unlike with mirrors)
M = magnification
h' = image height [m]
h = object height [m]
Constructive and Destructive Interference by Single
and Double Slit Defraction and Circular Aperture
Young’s double-slit experiment (bright fringes/dark fringes):
Double Slit
Constructive:
∆L d m= =sinθ λ
Destructive:
∆L d m= = +sin ( )θ λ1
2
d = distance between the slits [m]
θ = the angle between a normal
line extending from midway
between the slits and a line
extending from the midway
point to the point of ray
Intensity:
I Im=





(cos )
sin2
2
β
α
α
β
π
λ
θ=
d
sin
α
π
λ
θ=
a
sin
Single-Slit
Destructive:
a msinθ λ=
Circular Aperture
1st
Minimum:
sin .
.
θ
γ
=122
dia
intersection.
m = fringe order number [integer]
λ = wavelength of the light [m]
a = width of the single-slit [m]
∆L = the difference between the
distance traveled of the two
rays [m]
I = intensity @ θ [W/m2
]
Im = intensity @ θ = 0 [W/m2
]
d = distance between the slits [m]
In a circular aperture, the 1st
minimum is the point at which
an image can no longer be
resolved.
A reflected ray undergoes a phase shift of 180°
when the reflecting material has a greater index of
refraction n than the ambient medium. Relative to the
same ray without phase shift, this constitutes a path
difference of λ/2.
Interference between Reflected and Refracted rays
from a thin material surrounded by another medium:
Constructive:
2 1
2nt m= +( )λ
Destructive:
2nt m= λ
t = thickness of the material [m]
m = fringe order number [integer]
λ = wavelength of the light [m]
If the thin material is between two different media, one with a
higher n and the other lower, then the above constructive
and destructive formulas are reversed.
Wavelength within a medium:
λ
λ
n
n
=
c n fn= λ
λ = wavelength in free space [m]
λn = wavelength in the medium [m]
c = the speed of light 3.00 × 10
8
[m/s]
f = frequency [Hz]
Polarizing Angle: by Brewster’s Law, the angle of
incidence that produces complete polarization in the
reflected light from an amorphous material such as glass.
tanθB
n
n
= 2
1
θ θr B+ = °90
θB = angle of incidence
producing a 90° angle
between reflected and
refracted rays.
θr = angle of incidence of the
refracted ray.
partially polarized
θr
n
2
1
nn
θbθb
non-polarized
Source
polarized
Intensity of light passing through a polarizing lense:
[Watts/m2
]
initially unpolarized: I I= 1
2 0
initially polarized:
I I= 0
2
cos θ
I = intensity [W/m
2
]
I0 = intensity of source [W/m
2
]
θ = angle between the polarity
of the source and the lens.
Tom Penick tomzap@eden.com www.teicontrols.com/notes 1/31/99

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